Compact short back focus imaging lens system with two lenses
a short back focus and imaging lens technology, applied in the field of compact short back focus imaging lens system with two lenses, can solve the problems of reducing the overall length of these imaging lens systems, affecting the quality of the image, and the difficulty of adjusting the focal length of the imaging lens, so as to achieve short back focal length, short overall length, and low cost
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first embodiment
The First Embodiment
Refer to FIG. 2-5, show the optical path and field curvature, distortion and vertical aberration (while radius is 0.6086 mm) of image of this embodiment, respectively.
List 1:fs = 3.408SurfaceLensRdNdυdObject∞1(Stop)*R10.94510.8311.58760.02*R21.47490.6063*R3−2.60891.1331.58760.04*R4−4.23560.3305R5∞0.5001.51764.176R6∞0.363Image∞*aspherical surface
List 2:KA4A6A8A10A12A14*R17.2509E−02−1.2766E−011.7993E+00−1.4137E+015.9805E+01−1.3135E+021.1763E+02*R28.4914E+004.4620E−025.4374E−01−1.5469E+004.1302E+00−2.4597E+000.0000E+00*R31.4394E+01−1.8524E−01−5.0197E−011.1023E+00−1.9051E+000.0000E+000.0000E+00*R41.8819E+00−2.8780E−02−8.5916E−02−3.1650E−022.2916E−01−2.6495E−011.2800E−01
In this embodiment, the first lens 11 and the second lens 12 are made from the same glass with the refractive index Nd of 1.587 and Abbe's number νd1 of 60.0. The IR cut-off filter 13 is made from glass with the refractive index Nd of 1.517 and Abbe's number νd1 of 64.17.
The fs is 3.408 mm, f1 is 2.787...
second embodiment
The Second Embodiment
Refer to FIG. 2&FIG. 6-8.
List 3fs = 3.129SurfaceLensRdNdυdObject∞1(Stop)*R10.93710.8241.58760.02*R21.50000.4523*R3−3.32051.0851.58760.04*R4−3.89010.3135R5∞0.7001.51764.176R6∞0.222Image∞*aspherical surface
List 4KA4A6A8A10A12A14*R13.0726E−01−1.2599E−011.8009E+00−1.4144E+015.9403E+01−1.3158E+021.2121E+02*R22.2171E+004.1705E−025.4018E−01−1.5075E+008.2928E+00−6.5863E+000.0000E+00*R31.2770E+01−1.8944E−01−5.1639E−011.0845E+00−2.4199E+000.0000E+000.0000E+00*R41.5449E+01−3.0803E−02−8.6594E−02−3.2235E−022.2793E−01−2.6552E−011.2771E−01
In this embodiment, the first lens 11 and the second lens 12 are made from the same glass with the refractive index Nd of 1.587 and Abbe's number νd1 of 60.0. The IR cut-off filter 13 is made from glass with the refractive index Nd of 1.517 and Abbe's number νd1 of 64.17.
The fs is 3.129 mm, f1 is 2.7719 mm, f2 is −130.8 mm, TL is 3.5959 mm, satisfying from the equation (1) to the equation (4).
d2+d4+d6fs=0.3155;f1f2=-0.0212;bfTL=0.3946;(R2-R3)...
third embodiment
The Third Embodiment
Refer to FIG. 2&FIG. 9-11.
List 5fs = 2.878Surface$L$ensRdNdυdObject∞1(Stop)*R10.86970.6921.58058.92*R21.53530.5123*R3−4.73621.1251.58058.94*R4−19.04320.1005R5∞0.7001.51764.176R6∞0.222Image∞*aspherical surface
List 6KA4A6A8A10A12A14*R11.6398E−01−1.2320E−018.7112E−01−3.7158E+002.6497E+002.7326E+002.0840E+01*R26.0971E+002.6171E−01−1.6968E+001.1420E+01−4.2238E+00−1.1136E+022.2379E+02*R3−3.1297E+02−2.7133E−01−1.7717E+007.9263E+00−9.4245E+00−4.5828E+011.4460E+02*R48.5842E+01−4.8528E−02−1.0180E−017.5329E−02−2.6834E−02−1.0559E−04−3.8768E−04
In this embodiment, the first lens 11 and the second lens 12 are made from the same glass with the refractive index Nd of 1.580 and Abbe's number νd1 of 58.9. The IR cut-off filter 13 is made from glass with the refractive index Nd of 1.517 and Abbe's number νd1 of 64.17.
The fs is 2.878 mm, f1 is 2.4924 mm, f2 is −11.1504 mm, TL is 3.3509 mm, satisfying from the equation (1) to the equation (4).
d2+d4+d6fs=0.2898;f1f2=-0.2235;bfTL=0.3551...
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